By looking at the pseudoscalar-vector meson spectra in the B¯→J/ψρK̄ and B¯→J/ψK̄∗π weak decays, we theoretically investigate the double-pole structure of the K1(1270) resonance by using the chiral unitary approach to account for the final-state interactions between the pseudoscalar (P) and vector (V) mesons. The K1(1270) resonance is dynamically generated through these interactions in coupled channels and influences the shape of the invariant mass distributions under consideration. We show how these shapes are affected by the K1(1270) double-pole structure to confront the results from our model with future experiments that might investigate the PV spectra in these decays
We evaluate ratios of the χc1 decay rates to η (η′, K-) and one of the f0(1370), f0(1710), f2(1270),...
We show that the τ− decay into f1(1285)π−ντ is dominated by a triangle loop mechanism with K⁎, K¯⁎ a...
Abstract We calculate the shape of the π and K ̄ N invari-ant mass distributions in the b → J/ψ π ...
Within the chiral unitary approach, the axial-vector resonance K1(1270) has been predicted to manife...
We analyze theoretically the D→ νeρK¯ and D→ νeK¯ π decays to see the feasibility to check the doubl...
We study theoretically the decay τ-→ντP-A, with P- a π- or K- and A an axial-vector resonance b1(123...
The axial-vector meson K1(1270) was studied within the chiral unitary approach, where it was shown t...
We analyze theoretically the $$D^+\rightarrow \nu e^+ \rho \bar{K}$$ and $$D^+\rightarrow \nu e^+ \b...
We study the τ→ νA decay, with A an axial-vector meson. We produce the a(1260) and b(1235) resonance...
We study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). The theore...
We study the decay of dynamically generated resonances from the interaction of two vectors into a γ ...
We perform a theoretical study of the χ→ϕKK¯→ϕKπK¯ reaction taking into account the KK¯ final state ...
We study the decay of dynamically generated resonances from the interaction of two vectors into a γ ...
AbstractWe study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). Th...
AbstractWe describe the B0 and Bs0 decays into J/ψ f0(500) and J/ψ f0(980) by taking into account th...
We evaluate ratios of the χc1 decay rates to η (η′, K-) and one of the f0(1370), f0(1710), f2(1270),...
We show that the τ− decay into f1(1285)π−ντ is dominated by a triangle loop mechanism with K⁎, K¯⁎ a...
Abstract We calculate the shape of the π and K ̄ N invari-ant mass distributions in the b → J/ψ π ...
Within the chiral unitary approach, the axial-vector resonance K1(1270) has been predicted to manife...
We analyze theoretically the D→ νeρK¯ and D→ νeK¯ π decays to see the feasibility to check the doubl...
We study theoretically the decay τ-→ντP-A, with P- a π- or K- and A an axial-vector resonance b1(123...
The axial-vector meson K1(1270) was studied within the chiral unitary approach, where it was shown t...
We analyze theoretically the $$D^+\rightarrow \nu e^+ \rho \bar{K}$$ and $$D^+\rightarrow \nu e^+ \b...
We study the τ→ νA decay, with A an axial-vector meson. We produce the a(1260) and b(1235) resonance...
We study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). The theore...
We study the decay of dynamically generated resonances from the interaction of two vectors into a γ ...
We perform a theoretical study of the χ→ϕKK¯→ϕKπK¯ reaction taking into account the KK¯ final state ...
We study the decay of dynamically generated resonances from the interaction of two vectors into a γ ...
AbstractWe study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). Th...
AbstractWe describe the B0 and Bs0 decays into J/ψ f0(500) and J/ψ f0(980) by taking into account th...
We evaluate ratios of the χc1 decay rates to η (η′, K-) and one of the f0(1370), f0(1710), f2(1270),...
We show that the τ− decay into f1(1285)π−ντ is dominated by a triangle loop mechanism with K⁎, K¯⁎ a...
Abstract We calculate the shape of the π and K ̄ N invari-ant mass distributions in the b → J/ψ π ...